HOT WIRE MASS FLOW MEASUREMENT DEVICE FOR A HIGH TEMPERATURE GAS
The present invention relates to apparatus for measuring the mass
flow of a high temperature gas stream particularly but not exclusively for
such a gas stream in an exhaust system of a modern internal combustion
engine.
A known arrangement for measuring gas mass flow rate utilises a
measurement of the cooling effect of the gas on a heated element as it
flows over the element. Arrangements of this type are well known in the
field of internal combustion engines and are utilised in the ambient air
intake system.
However, such systems are not usually suitable for use with gases
such as are found in automotive engine exhaust systems, which gases are
hot, polluted and corrosive. In particular, pollutants in the exhaust gases
can be deposited as a layer onto the surface of the heated element. This
pollutant layer will affect the heat transfer properties between the heated
element and the gas and will therefore reduce the accuracy of
measurements of cooling effect made.
It is therefore an object of the present invention to provide an
arrangement for measuring gas mass flow rate that avoids these inherent
difficulties with the known arrangements.
Thus and in accordance with the present invention therefore there
is provided an apparatus for measuring the mass flow of a high
temperature gas stream, said apparatus comprising an electrical heating
element supplied with current from a current source, control means to
control the flow of current through the element from the source,
temperature measurement means to measure the temperature of gas in
the hot gas stream and mass flow rate calculation means to calculate the
mass flow rate wherein the flow of current through the element is
controlled by said control means to maintain said element at a
predetermined temperature, the predetermined temperature being greater
than the temperature of the gas in the hot gas stream and sufficient to
degrade deposits on the surface of the heating element, and a value for
said hot gas mass flow rate is determined by said calculation means from
the measured gas temperature and the amount of energy dissipated in
said element to maintain said predetermined temperature.
With this arrangement it is possible to measure gas mass flow rate
in a high temperature gas stream more efficiently and accurately and to
minimise the effects of pollutants in the gas on the measurement.
Preferably, the heating element is a resistor with a positive
temperature coefficient.
The apparatus may be adapted to measure the mass flow rate of an
exhaust gas stream of an engine, preferably an internal combustion
engine. In order to achieve this the heating element and the temperature
measurement means are positioned such that they project into the
exhaust gas stream. Preferably the engine has an engine control unit and
most preferably the engine control unit provides the current source,
control means and mass flow calculation means for the apparatus.
Alternatively, an independent electronic control unit may provide these
functions.
In some embodiments the heating element may be switched
between being maintained at a first predetermined temperature and being
maintained at a second predetermined temperature, in particular wherein
the first predetermined temperature is higher than the gas temperature
and is sufficient to degrade deposits on the surface of the heating
element and the second predetermined temperature is higher than the
temperature of the gas stream but is not high enough to degrade deposits
on the surface of the heating element. This allows the heating element to
operate at the lower second predetermined temperature at least part of
the time making the apparatus more reliable and to operate at the first
higher predetermined temperature in order to degrade deposits of
pollutants which form on the surface of the heating element. In typical
operation the heating element is maintained at the first predetermined
temperature for less time than it is maintained at the second
predetermined temperature.
The times at which the heating element is switched between the
first predetermined temperature and the second predetermined
temperature are determined according to any suitable function of time. In
a preferred embodiment, the heating element is maintained at the first
predetermined temperature for a time interval after being switched on and
then maintained at the second predetermined temperature thereafter. In a
particularly preferred embodiment the timing of the switching between the
first predetermined temperature and the second predetermined
temperature is determined from an integration of engine effort coefficient
calculated by the engine control unit.
The accuracy of the measurement of mass flow rate may be
affected by such parameters as the specific heat of the gas, the gas
pressure, including static gas pressure, engine speed, engine load, lambda
value and, where the arrangement is used in an internal combustion
engine, pressure pulsations caused by normal operation of the engine.
Accordingly correction factors may be used to adjust the value obtained
from a simple calculation of gas mass flow rate to account for these
parameters. Preferably storage means are provided in which suitable
correction factors may be stored.
The invention will now be described by way of example only and
with reference to the accompanying drawings, the single Figure of which
shows, in schematic form, one embodiment of arrangement for measuring
gas mass flow rate in accordance with the present invention.
Referring now the drawing, there is shown an arrangement for
measuring the mass flow rate of gas in a hot gas stream.
The arrangement comprises a heater element 101 mounted on an
exhaust system of an internal combustion engine. The element 101
projects internally of the exhaust system and extends into the exhaust
gas stream.
The element 101 is maintained at a constant temperature by
passing an electric current through it from a current source 201 . The
current source 201 in the embodiment shown is provided in an electronic
control unit 200 (ECU). The heater element 101 is preferably a positive
temperature coefficient resistor. The current passed through the
temperature coefficient resistor from the current source 201 is adjusted
by a control device 202 to maintain the resistance of the positive
coefficient resistor at a predetermined target value representing a target
temperature for the positive temperature coefficient resistor- The
instantaneous energy dissipated in the positive temperature coefficient
resistor can be determined from the instantaneous value of the current
and the target value of the resistance of the temperature coefficient
resistor and this represents the cooling effect of the air flow on the
heated temperature coefficient resistor. The temperature of the gas in the
gas stream is measured by any suitable temperature sensor 103 also
monitored in the exhaust gas stream. The temperature sensor 103 is
connected via a interface 203 to a mass flow rate calculation device 204
which is, in the embodiment shown, also provided in the ECU. The heater
element 101 is also connected to the calculation device via current source
201 and control means 202.
The cooling effect of the gas flow is a function of the mass flow
rate, the area of the positive temperature coefficient resistor in contact
with the gas flow and the difference between the temperature of the gas
in the hot stream and the temperature of the positive temperature
coefficient resistor. Therefore by appropriate calculation, the gas mass
flow rate can be calculated from these values in the calculation device.
In order to obtain greater accuracy in measurement of the mass
flow rate, the temperature of the gas is preferably measured at a point
where the effects of the heating of the positive temperature coefficient
resistor on the temperature of the gas are minimal and at an acceptable
level. Furthermore, it will be appreciated that the target temperature of
the positive temperature coefficient resistor must be higher than the
temperature of the gas in the hot stream by an amount large enough for
the cooling effect of the gas stream to be measured.
The area of the positive temperature coefficient resistor in contact
with the gas can be reduced by deposits of pollutant on the surface of the
heater. To reduce or eliminate the deposition of the pollutant onto the
surface of the positive temperature coefficient resistor, the positive
temperature coefficient resistor, is in the present invention, operated at a
temperature above that which pollutants are burnt off (the pollutant burn
off temperature). This will clearly avoid the problems associated with the
known arrangements where the pollutant deposits on the surface on the
heater effecting measurement. However, operation at high temperature
can have a deleterious effect on the reliability of the temperature
coefficient resistor itself and therefore, it is advantageous for the target
temperature to be adjusted to be above the pollutant burn off temperature
for only a part of the time and at a lower temperature for the remainder of
the operating time. In order to achieve this, the arrangement of the
invention may switch between these two temperatures as a simple
function of time. Alternatively, where the arrangement is incorporated in
an internal combustion engine, there may be one high temperature period
during which pollutants are burnt off the temperature resistor at every
engine start up. In a particularly preferred arrangement, the timing of
switching to the high temperature is determined from a calculated
"integration of engine effort" coefficient. This calculation is known in the
art and is based on time, engine speed, gear selection, throttle position
and other such parameters and is designed to predict the likelihood of
pollutant formation in the exhaust gases.
The deposition of pollutant on the temperature sensor which
measures the temperature of the gas in the hot gas stream is of lesser
importance since such a deposition does not effect accuracy but only the
response time of the sensor to temperature changes.
However, there are other parameters that can affect the accuracy
of the measurement of mass gas flow by the arrangement of the
invention. Such parameters include the specific heat of the gas, the static
pressure of the gas and, where the arrangement is used in an internal
combustion engine, pressure pulsations caused by normal operation of the
engine.
In these circumstances, it has been realised that correction factors
can be used to adjust the value obtained from a simple calculation of gas
mass flow rate to account for these parameters.
For example, the variation in specific heat between a 30: 1 air/fuel
ratio diesel exhaust gas and stoichiometric diesel exhaust gas is
approximately 5%. This can be compensated for by a factor derived from
a measurement of excess oxygen in the hot gas. In a preferred
embodiment therefore, the arrangement of the invention utilises a
compensation table which gives a correction factor for various values of
excess oxygen which is to be applied to be calculated gas mass flow rate.
Furthermore, the variation in static pressure of the hot gas can
affect the density of the gas and therefore the velocity at given flow
rates. To a lesser extent, it also affects the specific heat of the gas. The
arrangement of the invention, when used in a diesel engine, can be
compensated for by utilisation of a stored correction factor derived from
pressure measurements.
In the exhaust systems of internal combustion engines there is
often a pulsating variation in gas pressure brought about by the opening
and closing of the exhaust valves in the engine. These pressure
pulsations are a function of engine speed and load and their magnitude at
various speed and load points is repeatable. A compensation factor can
be determined for a range of speed and load values and can be stored in a
two-dimensional array in the arrangement of the invention.
It is preferred that mass flow sensors for use in the arrangement of
the invention are tested and calibrated in a test rig using test gases and
test gas temperatures before use. The mass flow sensors are calibrated
on the test rig and test results recorded. Parameters are calculated from
the measured test results that relate to the performance of the mass flow
sensor under the test conditions and are known by experimentation,
empirical knowledge or calculation to be capable of defining the
performance of one sensor relative to a standard sensor.
These parameters are then recorded. When the temperature sensor
is installed into an operating exhaust system, these parameters are
entered into a controlling engine control unit which assists in optimising
the performance of the temperature sensor. The parameter can be stored
in the engine control system and can be distributed with the temperature
sensor or can be acceptable at data points and made available via
communication means. The parameters may also be stored within non¬
volatile memory means which may form a part of the temperature sensor
itself.
It is of course to be understood that the invention is not intended
to be restricted to the details of the above embodiments which are
described by way of example only.